The medium modification to the heavy quark potential
can be obtained from the inverse Fourier transform of the
resummed gluon propagator
in the static limit as [1]}
\(V(r;T,B,\mu )= C_F~g^2\int \frac{d^3p}{(2\pi )^3}(e^{ip.r}-1)~D^{00}(p_0=0,p),\) 
